Electrodynamics of Continuous Media, Volume 8Covers the theory of electromagnetic fields in matter, and the theory of the macroscopic electric and magnetic properties of matter. There is a considerable amount of new material particularly on the theory of the magnetic properties of matter and the theory of optical phenomena with new chapters on spatial dispersion and non-linear optics. The chapters on ferromagnetism and antiferromagnetism and on magnetohydrodynamics have been substantially enlarged and eight other chapters have additional sections. |
From inside the book
Results 1-3 of 71
Page 63
... grad ɛ can be written as grad ɛ = ( λɛ / λT ) , grad T + ( dɛ / λp ) , grad p . Then ( 15.12 ) becomes Ρ θε f = - grad Po ( p , T ) + grad E2 8π [ ( C ) , ] - ( G ) , grad T. ( 15.15 ) If the temperature also is constant throughout the ...
... grad ɛ can be written as grad ɛ = ( λɛ / λT ) , grad T + ( dɛ / λp ) , grad p . Then ( 15.12 ) becomes Ρ θε f = - grad Po ( p , T ) + grad E2 8π [ ( C ) , ] - ( G ) , grad T. ( 15.15 ) If the temperature also is constant throughout the ...
Page 103
... grad T dv . ( 28.2 ) Like the electric current density , the diffusion flux may be written as a linear combination of E and grad , or of j and grad . Using the symmetry of the kinetic coefficients , we can relate one of the coefficients ...
... grad T dv . ( 28.2 ) Like the electric current density , the diffusion flux may be written as a linear combination of E and grad , or of j and grad . Using the symmetry of the kinetic coefficients , we can relate one of the coefficients ...
Page 127
... grad Po + - grad [ H2p ( 2 ) , ] - Ομ H2 8π μ grad μ - grad H2 + ( H⚫grad ) H . 8π By a well - known formula of vector analysis , ( H⚫grad ) H = Thus f = - grad Po + 8π grad H2 - H x curl H = grad H2 + 4лj × Н / c . = Ομ 11 Rrad [ H2p ...
... grad Po + - grad [ H2p ( 2 ) , ] - Ομ H2 8π μ grad μ - grad H2 + ( H⚫grad ) H . 8π By a well - known formula of vector analysis , ( H⚫grad ) H = Thus f = - grad Po + 8π grad H2 - H x curl H = grad H2 + 4лj × Н / c . = Ομ 11 Rrad [ H2p ...
Contents
ELECTROSTATICS OF CONDUCTORS 1 The electrostatic field of conductors 13892 | 1 |
2 The energy of the electrostatic field of conductors | 7 |
3 Methods of solving problems in electrostatics | 17 |
Copyright | |
118 other sections not shown
Other editions - View all
Electrodynamics of Continuous Media: Volume 8 L D Landau,E.M. Lifshitz,L. P. Pitaevskii Snippet view - 1995 |
Common terms and phrases
angle anisotropy anisotropy energy antiferromagnetic atoms averaging axes axis body boundary conditions calculation charge circuit coefficient components conductor constant coordinates corresponding cross-section crystal Curie point curl H denote depends derivative determined dielectric diffraction direction discontinuity dispersion E₁ electric field electromagnetic electrons ellipsoid expression external field factor ferroelectric ferromagnet field H fluctuations fluid flux formula free energy frequency function given gives grad H₁ H₂ Hence incident induction integral isotropic Laplace's equation linear magnetic field magnetic moment Maxwell's equations medium normal obtain optical particle permittivity perpendicular perturbation phase plane polarization PROBLEM propagated properties pyroelectric quantities refraction relation respect result rotation satisfied scattering sin² SOLUTION sphere suffixes superconducting surface symmetry temperature tensor theory thermodynamic potential transition uniaxial values variable velocity volume wave vector z-axis zero Απ